Polarization of high-energy electrons traversing a laser beam
arXiv:hep-ph/9706405 · doi:10.1016/S0168-9002(97)01114-5
Abstract
When polarized electrons traverse a region where the laser light is focused their polarization varies even if their energy and direction of motion are not changed. This effect is due to interference of the incoming electron wave and an electron wave scattered at zero angle. Equations are obtained which determine the variation of the electron density matrix, and their solutions are given. The change in the electron polarization depends not only on the Compton cross section but on the real part of the forward Compton amplitude as well. It should be taken into account, for example, in simulations of the conversion for future colliders.
11 pages, LaTeX , 2 postscript figures included
Cited by in corpus (7)
- TESLA Technical Design Report, Part VI, Chapter 1: The Photon Collider at TESLA
- Loops and polarization in strong-field QED
- Electron (positron) beam polarization by Compton scattering on circularly polarized laser photons
- Helicity transfer in strong laser fields via the electron anomalous magnetic moment
- Resummation of quantum radiation reaction and induced polarization
- Strong signature of one-loop self-energy in polarization resolved nonlinear Compton scattering
- Laser-driven lepton polarization in the quantum radiation-dominated reflection regime